US2711483A - Discriminator for proportional counters - Google Patents

Discriminator for proportional counters Download PDF

Info

Publication number
US2711483A
US2711483A US145946A US14594650A US2711483A US 2711483 A US2711483 A US 2711483A US 145946 A US145946 A US 145946A US 14594650 A US14594650 A US 14594650A US 2711483 A US2711483 A US 2711483A
Authority
US
United States
Prior art keywords
voltage
tube
detector
pulses
discriminator
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US145946A
Inventor
Herzog Gerhard
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Texaco Inc
Original Assignee
Texaco Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Texaco Inc filed Critical Texaco Inc
Priority to US145946A priority Critical patent/US2711483A/en
Application granted granted Critical
Publication of US2711483A publication Critical patent/US2711483A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/18Measuring radiation intensity with counting-tube arrangements, e.g. with Geiger counters
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03GCONTROL OF AMPLIFICATION
    • H03G3/00Gain control in amplifiers or frequency changers without distortion of the input signal
    • H03G3/20Automatic control
    • H03G3/22Automatic control in amplifiers having discharge tubes
    • H03G3/26Muting amplifier when no signal is present or when only weak signals are present, or caused by the presence of noise, e.g. squelch systems

Definitions

  • the present invention relates to the operation of radiation detectors of the counter type and more particularly to methods and circuits for the operation and control of such radiation detectors in the range in which they operate as proportional counters.
  • the present invention is particularly intended for use in applications in which the detector is subjected to radiations of varying types and in which it is desired to select and indicate or record responses due to certain types of radiation while eliminating those due to other types.
  • the invention is particularly applicable to the discriminatory indication or recording of the intensity of radiation due to alpha particles or to alpha particles and protons in the presence of radiation due to beta particles or gamma rays.
  • the invention may be employed, for example, in what is known as neutron well logging, in which it is desired to indicate or record the intensity of the scattered slow neutron radiation from structural formations bombarded by neutrons while eliminating or suppressing responses to gamma rays coming directly from the radiation source or being scattered by the surrounding material and also those due to natural or induced gamma rays from the formations.
  • neutron well logging in which it is desired to indicate or record the intensity of the scattered slow neutron radiation from structural formations bombarded by neutrons while eliminating or suppressing responses to gamma rays coming directly from the radiation source or being scattered by the surrounding material and also those due to natural or induced gamma rays from the formations.
  • the detectors employed are of the counter or pulse producing type and are operated in a range of applied voltage in which the size or amplitude of the pulses varies with the initial ionization caused by the radiation or particle producing the pulse; i. e., in what is known as the proportional counter range.
  • the counter is sensitized so that the slow neutrons or a certain proportion thereof passing through the field in which the counter is located will produce ionizing particles.
  • Such sensitization is effected, for example, by coating the cathode elements of the detector with boron or lithium compounds, for example, boron carbide, or by employing within the detector a vapor or gaseous filling which includes boron fluoride.
  • bombardment with slow neutrons will cause the production of alpha particles from the isotopes of the boron or lithium compound used for sensitizing the detector.
  • the detector is at the same time sensitive to gamma rays, bombardment with which causes emission of beta particles. Thus the detector produces pulses as a result of the impingement of both slow neutrons and gamma rays.
  • a detector suitable for use in accordance with the present invention is shown in the U. S. Letters Patent No. 2,462,471 granted to K. C. Crumrine, February 22, 1949.
  • the pulses resulting from the action of the slow neutrons are of greater size or amplitude than those United States Patent 0 ice resulting from the action of gamma rays when the detector is operated in the proportional counter range; that is, under applied voltages below those of the operating range of the Geiger-Mueller counter, in which the size of the pulses becomes substantially independent of the initial ionization of the particles producing them.
  • Difliculty arises in the use of radiation detectors in the proportional counter range and particularly in such discriminatory use as is hereinbefore referred to, in that such counters aresensitive to even small changes in voltage applied across the electrodes of the detector, such changes resulting both in changes of pulse size or amplitude and in the number of pulses produced in a field of given intensity of radiation.
  • the operation of the detector and the discriminatory action of the circuits associated with it are stabilized at a predetermined level irrespective of ordinary fluctuations or changes in the voltage applied to the detector.
  • the detector is associated with an amplifier channel or circuit in which, preferably after direct linear amplification of the pulses derived from the detector, the pulses of less or amplitude than those due to the alpha rays are eliminated by control of the bias voltage on the control grid of one of the tubes in the amplifying circuit, generally a tube receiving positive pulses, produced by the detector which have been linearly amplified.
  • the grid bias of this tube may be pre-set so as to eliminate pulses with an amplitude less than a particular value at the normal and desired operating voltage at the counter, which may be, for example, 1100 volts.
  • the number of pulses passed by the discriminating amplifier is held constant irrespective of changes in voltage on the counter, assuming a constant neutron flux; or in other words, the changes in voltage are automatically compensated for in the operation of the discriminating system. This is effected by automatically changing the grid bias on the discriminating amplifier with changes in voltage on the counter.
  • the necessary change in the grid bias of the discriminator tube is effected by separately controlling the voltage applied to the cathode of the discriminator tube and that applied to the grid and varying the voltage applied to the grid inversely as a function of changes in the high voltage applied to the detector.
  • the numeral 10 indicates a detector, which may suitably be of the type described in the Crumrine Patent No. 2,462,471, above referred to, and which is sensitized so that it responds to slow neutron bombardment. It is shown schematically and, as is apparent, may be a single or multiple detector.
  • the cathode of the detector is shown as being grounded through the conductor 11.
  • the necessary voltage for operation of the detector is supplied from a suitable high voltage source through the conductor 12 and the resistor 13.
  • the detector is operated with the applied high voltage across its electrodes of an order such that it acts as a proportional counter.
  • this voltage may be in the order of 600 to 1200 volts.
  • the intended range of operation is in the order of 1100 volts.
  • the gamma rays which cause the emission of beta particles in the detector result in pulses of smaller magnitude; and slow neutrons, which cause the emission of alpha particles from the sensitizing material used in the detector, produce pulses of larger magnitude.
  • the pulses which are produced within the detector appear at the anode as negative pulses and are transmitted through coupling condenser 14 to an amplifier or amplifying train indicated at 15, in which they are linearly amplified and from which they are transmitted as positive amplified pulses through coupling condenser 16 to the grid 17 of the discriminating amplifier 18.
  • Suitable means for linearly amplifying and reversing the pulses from the detector are shown, for example, in the application of Crumrine, Serial No. 676,165, filed June 12, 1946, which matured as U. S. Patent No. 2,557,636.
  • a suitable discriminator circuit is illustrated in the righthand portion of the figure, in which means are provided for stabilizing the voltage on the cathode of the discriminator tube.
  • the tube 18, as used in the discriminator circuit, may be an amplifying tube having a high gain, such as a 6AC7 tube.
  • a suitable source of positive voltage for the plate 19 of the tube 18 may be connected to the conductor 20. The voltage for its operation is applied to the plate 19 through the resistor 21.
  • the cathode 22 of the tube 18 is connected to one end of a resistor 23, the other end of which is grounded.
  • the screen grid 24 of tube 18 is connected directly to the source of voltage applied to the plate 19.
  • the suppressor grid 25 is maintained at cathode voltage.
  • control grid 17 of the tube 18 is maintained at a voltage negative to that on the cathode 22, this negative or bias voltage being such as to prevent the tube from delivering pulses other than those resultingfrom the production of alpha particles in the detector produced by neutron bombardment.
  • the output of the tube 18 is delivered through coupling condenser 26 to any suitable amplifying, integrating, recording or counting device, not shown.
  • a similar tube 27 is placed in parallel to it, being connected between the source of voltage for the plate circuit of tube 18 and the resistor 23.
  • the plate 28 of tube 27 is directly connected to the conductor 20 upon which the voltage for operation of the plate circuit of the tube 13 is impressed although, if desired, a resistor of lower resistance than resistor 21 may be inserted in the line to the plate 28.
  • the tube 27 is operated as a triode, the screen and suppressor grids being maintained at plate voltage. A suitable triode may be used, if desired.
  • the cathode 29 of tube 27 is connected to the resistor 23,
  • the control grid 30 is connected to a stabilized source of positive voltage, by which there is impressed upon it a voltage but a few volts lower than that upon the cathode. Since both tubes 18 and 27 have the same cathode resistor 23, under normal operating conditions the cathode voltage which is developed by the two plate currents flowing through resistor 23 is substantially constant.
  • the tube 27 has ,no plate resistor and therefore passes a larger current than the discriminator tube 18 and thereby aids in maintaining the common cathode voltage on the cathodes of the two tubes substantially constant.
  • control of the bias on the control grid 17 of discriminator 18 as a function of the voltage of the source of high voltage 1 applied to the detector anode is efiected in the following manner:
  • a voltage divider is provided, one end of which is connected to a stabilized source of positive voltage and the other end to a point of lower voltage or being grounded, a suitable source of positive voltage therefor being that for the plate circuit of the discriminator tube.
  • a voltage divider is interposed between the source of positive voltage for the plate circuits of the tubes 13 and 27 and the ground, in parallel to those tubes, this voltage divider being made up of the resistor 31 and the potentiometer 32. From a point on the potentiometer 32 a tap 33 is connected through resistor 34 to the control grid 1'7.
  • the position of the tap 33 on potentiometer 32 is adjusted to give the desired bias voltage relative to cathode 22 on the control grid 17 to eliminate all but the desired pulses.
  • This voltage may suitably be 5 volts in a tube of the character hereinbefore referred to.
  • a conductor 36 leads to the plate of a control tube 37 which may suitably be a triode of relatively low gain such as a 615 tube.
  • a potentiometer 38 of high resistance is interposed in a circuit from the source of high voltage for the detector and the ground. From a suitable point on this potentiometer, a tap 39 leads to the control grid 40 of tube 37.
  • the cathode 41 of tube 37 is connected to a stabilized positive source of voltage.
  • the tap 39 on the potentiometer 38 is adjusted so that the control grid 40 of tube 37 is maintained under a slight negative bias relative to the cathode voltage.
  • the grid bias on the tube 18 becomes more negative. It may go, for example, from 5 to 6 volts. This increase in the negative bias on the control grid of the tube 18 results in a reduced output of pulses which may suitably be adjusted to give a substantially constant output of pulses irrespective of small changes in the high voltage applied to the detector, assuming a constant neutron flux.
  • the resistance of resistor 38 was 1 megohm.
  • the tube 37 was a 61 5 tube and the cathode was maintained at a constant voltage of +110 volts.
  • the resistance of resistor 31 was 100,000 ohms and that of potentiometer 32 was 50,000 ohms.
  • the resistance of grid resistor 34 was 1 megohm.
  • the tubes 18 and 27 were both 6AC7 tubes and the applied voltage for their plate circuits at the conductor 20 was +300 volts.
  • the resistance of plate resistor 21 was 7,000 ohms; that of the common cathode resistor 23 was 2400 ohms.
  • the cathodes of both tubes were maintained at +125 volts.
  • the control grid 30 of tube 27 was maintained at +120 volts.
  • an amplifying and selecting circuit for use with a radiation detector delivering pulses of diflerent sizes resulting from different types of radiation, and including discriminating means comprising an electron discharge tube having its control grid coupled to receive amplified positive pulses derived from such detector and with a voltage on said grid less than that on the cathode of said tube to provide a negative grid bias and thereby cause said tube to select and transmit substantially only pulses of larger amplitude, means for controlling the action of said discriminator and for compensating for changes in its output due to changes in the high voltage impressed upon said detector, said control means comprising a direct current voltage divider to which a constant positive voltage is applied and including at least two resistors in series, at least a part of the resistor at lower voltage being in the control grid circuit of the discriminator tube to provide biasing voltage therefor, and means controlling the voltage impressed on said resistor as an inverse function of the voltage impressed upon the detector to correspondingly vary the grid bias of the discriminator tube, said means comprising an electron discharge tube having its plate connected to said voltage

Description

June 21, 1955 HERZOG 2,711,483
I DISCRIMINATOR FOR PROPORTIONAL COUNTERS Filed Feb. 24, 1950 k w S m 1 a N W, k x; R}
f 3 w s w INVENTOR.
DISCRIIVIINATOR FOR PROPORTIONAL C(IUNTERS Gerhard Herzog, Houston, Tex., assignor to The Texas Company, New York, N. Y., a corporation of Delaware Application February 24, 1950, Serial No. 145,946
2 Claims. c1. 25083.6)
The present invention relates to the operation of radiation detectors of the counter type and more particularly to methods and circuits for the operation and control of such radiation detectors in the range in which they operate as proportional counters. The present invention is particularly intended for use in applications in which the detector is subjected to radiations of varying types and in which it is desired to select and indicate or record responses due to certain types of radiation while eliminating those due to other types. Thus the invention is particularly applicable to the discriminatory indication or recording of the intensity of radiation due to alpha particles or to alpha particles and protons in the presence of radiation due to beta particles or gamma rays. The invention may be employed, for example, in what is known as neutron well logging, in which it is desired to indicate or record the intensity of the scattered slow neutron radiation from structural formations bombarded by neutrons while eliminating or suppressing responses to gamma rays coming directly from the radiation source or being scattered by the surrounding material and also those due to natural or induced gamma rays from the formations.
In connection with the present invention, the detectors employed are of the counter or pulse producing type and are operated in a range of applied voltage in which the size or amplitude of the pulses varies with the initial ionization caused by the radiation or particle producing the pulse; i. e., in what is known as the proportional counter range. When slow neutrons are to be detected, the counter is sensitized so that the slow neutrons or a certain proportion thereof passing through the field in which the counter is located will produce ionizing particles. Such sensitization is effected, for example, by coating the cathode elements of the detector with boron or lithium compounds, for example, boron carbide, or by employing within the detector a vapor or gaseous filling which includes boron fluoride. When so sensitized, bombardment with slow neutrons will cause the production of alpha particles from the isotopes of the boron or lithium compound used for sensitizing the detector.
The detector is at the same time sensitive to gamma rays, bombardment with which causes emission of beta particles. Thus the detector produces pulses as a result of the impingement of both slow neutrons and gamma rays. A detector suitable for use in accordance with the present invention is shown in the U. S. Letters Patent No. 2,462,471 granted to K. C. Crumrine, February 22, 1949.
It is frequently desired to separately indicate or record the responses or pulses due to slow neutrons while eliminating the efiect of those due to the gamma rays. Since the alpha particles resulting from slow neutron bombardment produce a greater initial ionization than the beta particles resulting from gamma ray bombardment, the pulses resulting from the action of the slow neutrons are of greater size or amplitude than those United States Patent 0 ice resulting from the action of gamma rays when the detector is operated in the proportional counter range; that is, under applied voltages below those of the operating range of the Geiger-Mueller counter, in which the size of the pulses becomes substantially independent of the initial ionization of the particles producing them.
Difliculty arises in the use of radiation detectors in the proportional counter range and particularly in such discriminatory use as is hereinbefore referred to, in that such counters aresensitive to even small changes in voltage applied across the electrodes of the detector, such changes resulting both in changes of pulse size or amplitude and in the number of pulses produced in a field of given intensity of radiation. In accordance with the present invention, the operation of the detector and the discriminatory action of the circuits associated with it are stabilized at a predetermined level irrespective of ordinary fluctuations or changes in the voltage applied to the detector.
In accordance with the present invention, the detector is associated with an amplifier channel or circuit in which, preferably after direct linear amplification of the pulses derived from the detector, the pulses of less or amplitude than those due to the alpha rays are eliminated by control of the bias voltage on the control grid of one of the tubes in the amplifying circuit, generally a tube receiving positive pulses, produced by the detector which have been linearly amplified. The grid bias of this tube may be pre-set so as to eliminate pulses with an amplitude less than a particular value at the normal and desired operating voltage at the counter, which may be, for example, 1100 volts. Assuminga constant neutron flux, if the voltage on the counter be increased somewhat, say to 1110 volts, the amplitudes of the pulses formed within the counter as well as the number of detectable pulses is increased. So likewise, if the voltage on the counter should decrease somewhat, say to 1090 volts, there will be a decrease in amplitude and number of pulses generated within the counter.
In accordance with the present invention, the number of pulses passed by the discriminating amplifier is held constant irrespective of changes in voltage on the counter, assuming a constant neutron flux; or in other words, the changes in voltage are automatically compensated for in the operation of the discriminating system. This is effected by automatically changing the grid bias on the discriminating amplifier with changes in voltage on the counter.
In accordance with the present invention, the necessary change in the grid bias of the discriminator tube is effected by separately controlling the voltage applied to the cathode of the discriminator tube and that applied to the grid and varying the voltage applied to the grid inversely as a function of changes in the high voltage applied to the detector. 7
The invention will be fully understood from the following description of a circuit embodying the invention, as illustrated schematically in the single figure of the drawings.
In the drawing, the numeral 10 indicates a detector, which may suitably be of the type described in the Crumrine Patent No. 2,462,471, above referred to, and which is sensitized so that it responds to slow neutron bombardment. It is shown schematically and, as is apparent, may be a single or multiple detector. The cathode of the detector is shown as being grounded through the conductor 11. The necessary voltage for operation of the detector is supplied from a suitable high voltage source through the conductor 12 and the resistor 13.
As has been pointed out above, the detector is operated with the applied high voltage across its electrodes of an order such that it acts as a proportional counter. Thus, for a detector of the type illustrated in the prior Crumrine application above referred to, this voltage may be in the order of 600 to 1200 volts. In the circuit illustrated and described herein, the intended range of operation is in the order of 1100 volts. The gamma rays which cause the emission of beta particles in the detector result in pulses of smaller magnitude; and slow neutrons, which cause the emission of alpha particles from the sensitizing material used in the detector, produce pulses of larger magnitude.
The pulses which are produced within the detector appear at the anode as negative pulses and are transmitted through coupling condenser 14 to an amplifier or amplifying train indicated at 15, in which they are linearly amplified and from which they are transmitted as positive amplified pulses through coupling condenser 16 to the grid 17 of the discriminating amplifier 18. Suitable means for linearly amplifying and reversing the pulses from the detector are shown, for example, in the application of Crumrine, Serial No. 676,165, filed June 12, 1946, which matured as U. S. Patent No. 2,557,636. A suitable discriminator circuit is illustrated in the righthand portion of the figure, in which means are provided for stabilizing the voltage on the cathode of the discriminator tube.
Such a circuit is illustrated, for example, in the paper by W. H. Jordan and P. R. Bell, Review of Scientific Instruments, volume 18, page 703 (October 1947).
The tube 18, as used in the discriminator circuit, may be an amplifying tube having a high gain, such as a 6AC7 tube. A suitable source of positive voltage for the plate 19 of the tube 18 may be connected to the conductor 20. The voltage for its operation is applied to the plate 19 through the resistor 21. The cathode 22 of the tube 18 is connected to one end of a resistor 23, the other end of which is grounded. The screen grid 24 of tube 18 is connected directly to the source of voltage applied to the plate 19. The suppressor grid 25 is maintained at cathode voltage. By means hereinafter described, the control grid 17 of the tube 18 is maintained at a voltage negative to that on the cathode 22, this negative or bias voltage being such as to prevent the tube from delivering pulses other than those resultingfrom the production of alpha particles in the detector produced by neutron bombardment. The output of the tube 18 is delivered through coupling condenser 26 to any suitable amplifying, integrating, recording or counting device, not shown.
In order to maintain the cathode voltage of the discriminator tube 18 constant a similar tube 27 is placed in parallel to it, being connected between the source of voltage for the plate circuit of tube 18 and the resistor 23. The plate 28 of tube 27 is directly connected to the conductor 20 upon which the voltage for operation of the plate circuit of the tube 13 is impressed although, if desired, a resistor of lower resistance than resistor 21 may be inserted in the line to the plate 28. The tube 27 is operated as a triode, the screen and suppressor grids being maintained at plate voltage. A suitable triode may be used, if desired. The cathode 29 of tube 27 is connected to the resistor 23, The control grid 30 is connected to a stabilized source of positive voltage, by which there is impressed upon it a voltage but a few volts lower than that upon the cathode. Since both tubes 18 and 27 have the same cathode resistor 23, under normal operating conditions the cathode voltage which is developed by the two plate currents flowing through resistor 23 is substantially constant. The tube 27 has ,no plate resistor and therefore passes a larger current than the discriminator tube 18 and thereby aids in maintaining the common cathode voltage on the cathodes of the two tubes substantially constant.
In accordance with the present invention, the control of the bias on the control grid 17 of discriminator 18 as a function of the voltage of the source of high voltage 1 applied to the detector anode is efiected in the following manner:
A voltage divider is provided, one end of which is connected to a stabilized source of positive voltage and the other end to a point of lower voltage or being grounded, a suitable source of positive voltage therefor being that for the plate circuit of the discriminator tube. In the illustrative circuit shown, a voltage divider is interposed between the source of positive voltage for the plate circuits of the tubes 13 and 27 and the ground, in parallel to those tubes, this voltage divider being made up of the resistor 31 and the potentiometer 32. From a point on the potentiometer 32 a tap 33 is connected through resistor 34 to the control grid 1'7. The position of the tap 33 on potentiometer 32 is adjusted to give the desired bias voltage relative to cathode 22 on the control grid 17 to eliminate all but the desired pulses. This voltage may suitably be 5 volts in a tube of the character hereinbefore referred to.
From an intermediate point 35 in the voltage divider between the resistor 31 and the potentiometer 32, a conductor 36 leads to the plate of a control tube 37 which may suitably be a triode of relatively low gain such as a 615 tube. A potentiometer 38 of high resistance is interposed in a circuit from the source of high voltage for the detector and the ground. From a suitable point on this potentiometer, a tap 39 leads to the control grid 40 of tube 37. The cathode 41 of tube 37 is connected to a stabilized positive source of voltage. The tap 39 on the potentiometer 38 is adjusted so that the control grid 40 of tube 37 is maintained under a slight negative bias relative to the cathode voltage.
As will be apparent, in the circuit as described changes in the high voltage supplied to the detector will be substantially immediately reflected in the operation of the discriminator tube 18. Thus, it it be assumed that this voltage increases, then the voltage at the tap 39 on potentiometer 38 will be increased and since the cathode voltage of tube 37 is constant, the bias on the control grid will be decreased and this will be reflected in an increase in plate current through the tube 37. Thus, if the cathode voltage on the tube 37 be maintained at volts, and the normal voltage on the control grid is 108 volts, the bias on the grid is 2 volts. If now, an increase in voltage at the high voltage source results in an increase in the voltage on the grid to 109 volts, the bias on the tube is decreased to 1 volt and the plate current through the tube 37 will increase accordingly. This will result in a reduction in the positive voltage at the point 35 between the resistor 31 and the potentiometer 32 to which the plate of tube 37 is connected. The voltage at this point may, for example, drop from +140 volts to +130 volts. This produces a corresponding reduction in voltage at the point where the tap 33 contacts the potentiometer 32; for example, from volts to 119 volts. The voltage on the control grid 17 of tube 18 is thereby likewise reduced and since the cathode voltage is made constant at, for example,
volts, the grid bias on the tube 18 becomes more negative. It may go, for example, from 5 to 6 volts. This increase in the negative bias on the control grid of the tube 18 results in a reduced output of pulses which may suitably be adjusted to give a substantially constant output of pulses irrespective of small changes in the high voltage applied to the detector, assuming a constant neutron flux.
In a circuit of the character described, in a specific example, the resistance of resistor 38 was 1 megohm. The tube 37 was a 61 5 tube and the cathode was maintained at a constant voltage of +110 volts. The resistance of resistor 31 was 100,000 ohms and that of potentiometer 32 was 50,000 ohms. The resistance of grid resistor 34 was 1 megohm. The tubes 18 and 27 were both 6AC7 tubes and the applied voltage for their plate circuits at the conductor 20 was +300 volts. The resistance of plate resistor 21 was 7,000 ohms; that of the common cathode resistor 23 was 2400 ohms. The cathodes of both tubes were maintained at +125 volts. The control grid 30 of tube 27 was maintained at +120 volts.
With this circuit, with a constant neutron flux and with an applied voltage across the counter of 1100 volts,
it was possible to maintain a substantially constantcounting rate in the range from 75,000 to 80,000 counts per minute for the output of the discriminator tube with variations of volts in either direction in the voltage applied to the detector anode; that is, in the range from 1090 volts to 1110 volts, whereas in the discriminator circuit without the improved control as hereinbefore described, variations to the same extent in the voltage applied to the counter were directly reflected in variations in the counting rate.
Although the present invention has been described in connection with the specific details of an illustrative example thereof, it is to be understood that these details are not to be regarded as limitations upon the scope of the invention except insofar as included in the accompanying claims.
I claim:
1. In an amplifying and selecting circuit for use with a radiation detector delivering pulses of diflerent sizes resulting from different types of radiation, and including discriminating means comprising an electron discharge tube having its control grid coupled to receive amplified positive pulses derived from such detector and with a voltage on said grid less than that on the cathode of said tube to provide a negative grid bias and thereby cause said tube to select and transmit substantially only pulses of larger amplitude, means for controlling the action of said discriminator and for compensating for changes in its output due to changes in the high voltage impressed upon said detector, said control means comprising a direct current voltage divider to which a constant positive voltage is applied and including at least two resistors in series, at least a part of the resistor at lower voltage being in the control grid circuit of the discriminator tube to provide biasing voltage therefor, and means controlling the voltage impressed on said resistor as an inverse function of the voltage impressed upon the detector to correspondingly vary the grid bias of the discriminator tube, said means comprising an electron discharge tube having its plate connected to said voltage divider at an intermediate point, the control a radiation detector delivering pulses of different sizes resulting from difierent types of radiation, and including I discriminating means comprising an electron discharge tube having its control grid coupled to receive amplified positive pulses derived from such detector and with a voltage on said grid less than on the cathode of said tube to provide a negative grid bias and thereby cause said tube to select and transmit substantially only pulses of larger amplitude, means for controlling the action of said discriminator and for compensating for changes in its'output due to changes in the high voltage impressed upon said detector, said control means comprising a direct current voltage divider shunted across the power supply of the discriminator tube and including at least two resistors in series, at least a part of the resistor at lower voltage being in the control grid circuit of the discriminator tube to provide biasing voltage therefor, and means controlling the voltage impressed on said resistor as an inverse function of the voltage impressed upon the detector to correspondingly vary the grid bias of the discriminator tube, said means comprising an electron discharge tube having its plate connected to said voltage divider between said two resistors, a resistor connected to the high voltage source for the detector, the
grid of said control tube being connected to said resistor and thereby deriving its voltage from the high voltage applied to the detector, whereby variations in the said high voltage cause inverse variations in the voltage applied to the lower voltage resistor of said voltage divider and in the voltage on the control grid of the discriminator tube.
References Cited in the file of this patent UNITED STATES PATENTS 2,310,342 Artzt Feb. 9, 1943 2,363,361 Reiskind Nov. 21, 1944 2,418,892. Lord, Jr. Apr. 15, 1947 2,443,857 Herzog June 22, 1948 2,465,938 Shonka Mar. 29, 1949 2,496,909 Eberhard Feb. 7, 1950 2,556,074 Eberhard June 5, 1951
US145946A 1950-02-24 1950-02-24 Discriminator for proportional counters Expired - Lifetime US2711483A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US145946A US2711483A (en) 1950-02-24 1950-02-24 Discriminator for proportional counters

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US145946A US2711483A (en) 1950-02-24 1950-02-24 Discriminator for proportional counters

Publications (1)

Publication Number Publication Date
US2711483A true US2711483A (en) 1955-06-21

Family

ID=22515250

Family Applications (1)

Application Number Title Priority Date Filing Date
US145946A Expired - Lifetime US2711483A (en) 1950-02-24 1950-02-24 Discriminator for proportional counters

Country Status (1)

Country Link
US (1) US2711483A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2837655A (en) * 1953-08-28 1958-06-03 Philips Corp X-ray fluorescent analysis apparatus
US2883551A (en) * 1954-08-20 1959-04-21 George V Zito High voltage generator
US2968728A (en) * 1955-11-18 1961-01-17 Eberline Instr Division Of Rey Underground exploration apparatus
US4365159A (en) * 1980-11-03 1982-12-21 The United States Of America As Represented By The Secretary Of The Navy Lithium-6 foil neutron detector
FR2508656A1 (en) * 1981-06-30 1982-12-31 Irt Corp PROPORTIONAL COUNTER OF LARGE AREA NEUTRONS AND OUTPUT CONTROLLER DETECTOR

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2310342A (en) * 1940-11-29 1943-02-09 Rca Corp Balanced direct and alternating current amplifiers
US2363361A (en) * 1942-10-26 1944-11-21 Rca Corp Control track stabilizing method and system
US2418892A (en) * 1945-04-24 1947-04-15 Texas Co Radiation detector quenching circuit
US2443857A (en) * 1945-04-24 1948-06-22 Texas Co Circuits for the control of radiation detectors
US2465938A (en) * 1946-11-21 1949-03-29 Francis R Shonka Radiation measuring device
US2496909A (en) * 1947-10-01 1950-02-07 Rca Corp Pulse amplitude discrimination
US2556074A (en) * 1947-10-29 1951-06-05 Rca Corp Pulse width selection

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2310342A (en) * 1940-11-29 1943-02-09 Rca Corp Balanced direct and alternating current amplifiers
US2363361A (en) * 1942-10-26 1944-11-21 Rca Corp Control track stabilizing method and system
US2418892A (en) * 1945-04-24 1947-04-15 Texas Co Radiation detector quenching circuit
US2443857A (en) * 1945-04-24 1948-06-22 Texas Co Circuits for the control of radiation detectors
US2465938A (en) * 1946-11-21 1949-03-29 Francis R Shonka Radiation measuring device
US2496909A (en) * 1947-10-01 1950-02-07 Rca Corp Pulse amplitude discrimination
US2556074A (en) * 1947-10-29 1951-06-05 Rca Corp Pulse width selection

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2837655A (en) * 1953-08-28 1958-06-03 Philips Corp X-ray fluorescent analysis apparatus
US2883551A (en) * 1954-08-20 1959-04-21 George V Zito High voltage generator
US2968728A (en) * 1955-11-18 1961-01-17 Eberline Instr Division Of Rey Underground exploration apparatus
US4365159A (en) * 1980-11-03 1982-12-21 The United States Of America As Represented By The Secretary Of The Navy Lithium-6 foil neutron detector
FR2508656A1 (en) * 1981-06-30 1982-12-31 Irt Corp PROPORTIONAL COUNTER OF LARGE AREA NEUTRONS AND OUTPUT CONTROLLER DETECTOR

Similar Documents

Publication Publication Date Title
US2481014A (en) Method and apparatus for radioactivity well logging
US3869608A (en) Nuclear well logging
US2576100A (en) Voltage stabilizing system and tube
US2550106A (en) Detector for elementary particles
US2758217A (en) Automatic scintillation counter
US2711483A (en) Discriminator for proportional counters
Fischer et al. The 6BN6 Gated‐Beam Tube as a Fast Coincidence Circuit
US2778947A (en) Automatic proportional counter
US2956165A (en) Borehole apparatus
US3183353A (en) Gain-stabilized scintiliation detection system
US2443857A (en) Circuits for the control of radiation detectors
US2644891A (en) Method of neutron borehole logging
US2968726A (en) Radiation measuring instrument
US2796533A (en) Logarithmic count rate or frequency meter
US2728862A (en) Radiation measuring instrument
US2750513A (en) Nuclear radiation measuring instrument
US2499311A (en) Neutron detection
GB2092841A (en) Neutron generator tube ion sourve control apparatus
US2994776A (en) Stabilized borehole logging
US3184597A (en) Stabilized scintillation detector
US2662188A (en) Voltage stabilizing amplifier system for neutron detectors
US2967245A (en) Neutron source for well logging apparatus
US2418892A (en) Radiation detector quenching circuit
US3071689A (en) Nuclear measuring system
US2503730A (en) Amplifying and quenching circuits for radiation detectors